copyright 2004 - john sayles1 bonding and geometry review unit 8 chapters 9 and 10
TRANSCRIPT
Copyright 2004 - John Sayles 1
Bonding and Geometry
Review Unit 8
Chapters 9 and 10
Copyright 2004 - John Sayles 2
Chemical Bonding Atoms react in order to achieve a full outer shell
– “stability” refers to the inability to react
– Full outer shell is a low energy configuration
Three main strategies– Ionic bonding
• Metal and nonmetal, one gains/one loses, e-’s transferred
– Covalent bonding• Two nonmetals, both gain, e-’s shared
– Metallic bonding• Two metals, both lose, cations in sea of e-’s
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Ionic Bonding Metal loses e-’s, forms pos. cations Nonmetal gains e-’s, forms neg. anion Ionic bond is the electrostatic attraction between the
cation and anion– Only one variation; no double, etc…– To compare the strength of ionic bonds, use Coulomb– Five steps of the Born-Haber cycle
• Form gaseous metal atoms, gaseous nonmetal atoms• Form cations, anions• Form ionic bonds and ionic crystal
Special valences– Trans metals lose s e-’s first (+2) then d’s (Sc,Fe,Ag,Zn)– Pseudo TM’s lose p’s first, then d’s (Pb+2 or +4)
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Born-Haber Cycle for NaCI
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Na(s)
Na(g)
+
+
Step 1
Step 2 Step 5
Cl2(g)
Cl(g) ClŠ(g)
NaCl(s)Direct
route
Step 4
Na+(g)Step 3
21
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Properties of Ionic Compounds Crystalline, brittle
– Lattice energy = ionic bond = 400kJ/mol (Coulomb)
Solids at normal temps– VERY high MP’s and BP’s; no IMF’s, must break ionics
Soluble in polar solvents– “Ionic” is the ultimate in polar
– Ions are vigorously hydrated
Conduct in melt or solution– Chock full o’ ions
– Must be mobile, as in melt or sol’n
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Covalent Bonding Both nonmetal atoms need to gain e-’s Impossible, so best option is to share e-’s
– Nuclei are mutually attracted to the shared pair Many variations
– Multiple bonds• Share 2 or 3 pairs of e-’s• Stronger and shorter• First bond is , others are
– Polar vs. nonpolar• ∆ electronegativity cause uneven sharing• Makes molecule polar if geometry is asymmetrical
– Resonance involves bonds flipping– Network and coordinate bonds
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Covalent Bonding in the H2 Molecule
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Covalent Bond Properties Bond strength depends on
– Order (# of shared pairs)– Polarity (∆ eneg)– Environment (eneg neighbors weaken bonds)– Indicated by bond energy (which, ironically, ignore
polarity and environment) Length “inversely proportional” to strength Vibrational frequency
– Stronger bonds vibrate at higher frequency, just like guitar strings
– Basis for spectroscopy
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Bond Energies (in kJ/mol)
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T9_5
Single Bonds
Multiple Bonds
C N O S
HCNOSFClBrI
H
432411386459363565428362295
346305358272485327285213
167201Ń283313ŃŃ
142Ń190218201201
226284255217Ń
155249249278
240216208
190175 149
F Cl Br I
CC CC CN NN N
C NC NN OO2
C OC OS O (in SO2)S O (in SO3)
602835418942
615887607494
745 (799 in CO2)1072
532469
*Data are taken from J. E. Huheey, Inorganic Chemistry, 4d ed. (New York: Harper & Row, 1993), pp. A21-A34
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Properties of Covalent Cmpds Low MP’s and BP’s
– Only mess with IMF’s to melt or boil
Solubility depends on polarity of compound– Polar dissolve in polar solvents, vice-versa
Don’t conduct in any state, except for …– Acids
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Lewis Structures Great way to represent the e- arrangement in a
covalent molecule– Do the Have/Need thing to count bonds
• Atoms “need” 8 e- each, except H
• “Have” refers to outer shell e-’s only
– (need - have) ÷ 2 = number of bonds
– Arrange atoms with highest bond capacity in middle
– Use sticks and snakebites to represent bonding and nonbonding e- pairs
Do NH3, CO2, N2, CO3-2, PF5
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Metallic Bonding Both metals need to lose e-’s Both do lose, creating “sea of e-’s”
– Accounts for conductivity, flexibility, luster
Vary in strength, as do MP’s and BP’s Insoluble in all solvents
– Acids convert them to salts, which dissolve
Conduct in the solid and melt, with e- sea
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Delocalized Bonding in Sodium Metal
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VSEPR Valence Shell Electron Pair Repulsion model Great for determing geometry of molecule Doesn’t explain
– Equivalence of bonds made from non-equiv orbitals– Multiple bonding– Para and diamagnetism
Premises– Basic geometry due to need to spread e- pairs out– Nonbonding (lone) e- pairs need more room
• They’re delocalized
– Multiple bond treated as a single e- pair
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Application of VSEPR Draw Lewis structure Total e- pairs determine basic geometry
– Linear, trigonal planar, tetrahedral, trigonal bipyramid, octahedral
Consider # and location of lone e- pairs to pick the specific geometry– Keep in mind lone pairs occupy roomiest
positions– See models
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Basic Geometries
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Specific Geometries
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More Specific Geometries
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Valence Bond Model Supposes the formation of Hybrid Orbitals
– To explain the equivalence of bonds– Sp, sp2, sp3, dsp3, d2sp3
• Each hybridization corresponds to a basic geometry
– Hybrids hold 1st bonding e- pairs and lone e- pairs• All bonds start with the overlap of hybrids
– Forms a bond
• 2nd and 3rd bond due to overlap of unhybribized p’s– Forms a bond
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Hybrid Orbitals and Their Spatial Arrangements
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Bonding in H2O
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Bonds vs. Bonds Bonds
– The overlap of hybrids– Overlap is along bond axis– Stronger (lower energy), approx. 400 kJ/mole– Can swivel
Bonds– Overlap of unhybridized p orbitals– Overlap is of bond axis (above and below)– Weaker, approx. 70% of bond (~280kJ/mol)– Cannot swivel
• Creates cis- and trans- isomerism (geometric isomerism)
– Involved in resonance• e-’s not localized
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Sigma and Pi Bonds
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Bonding in Ethylene
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Bonding in Acetylene
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Valence Bond Model Designed to explain equivalence of bonds made
from nonequivalent orbitals– Throw s’s and p’s in the quantum blender to form
equivalent hybrids Also explains details of multiple bonding
– No “wink-wink” bogosity– Explains relative strengths of single, double, triple bonds
bonds not as strong as bonds
– Explains resonance• e-’s in p orbitals are delocalized
Does NOT explain para and diamagnetism
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Molecular Orbital Model Supposes the formation of molecular orbitals
– Not to be confused with hybrid atomic orbitals– Use QM to combine ’s atomic orbitals
Combining 2 atomic orbitals creates 2 molecular orbitals– One is lower in energy ---> bonding
• Putting e-’s here creates attraction
– One is higher in energy ---> anti-bonding• Putting e-’s here creates repulsion
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Formation of Bonding and Anti-bonding Orbitals from 1s Orbitals to Hydrogen Atoms
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Using the MO Model Create MO’s
– Draw the MO diagram (see following slides)
Fill MO’s using the Aufbau Principle– Lowest energy first
– Spread out e- among degenerate MO’s
– Only 2 e-’s per MO
Interpret MO diagram– Bond order = # bonding pairs - # antibonding pairs
– Paramagnetism requires at least one unpaired e-
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Relative Energies of 1s of the H atom and the sigma1s and sigma*1s Molecular Orbitals of H2
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Ene
rgy 1s
1s
1s
1s
H atom H atomH2 molecule
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The Energies of the Molecular Orbitals of Li2
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Li atom Li atom
En
erg
y2s
2s
2s
2s
1s
1s
1s
1s
Li2 molecule
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The Different Ways in Which 2p Orbitals can Interact
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Relative Energies of Molecular Orbitals of Homonuclear Diatomic Molecules (Excluding K Shells)
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2p 2p
2p
2p
2s
*2p
*2p
2s 2s*2s
Atom AtomMolecule
Ene
rgy
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Molecular Polarity In order for a molecule to be polar, it must
– Contain polar bonds• ∆ electronegativity
• Most bonds are at least a little polar
• Measured as dipole moment (in DeByes’s)
– And be asymmetrical
Polarity affects properties– IMF’s
– MP, BP, volatility, solubility, viscosity, surface tension